Pseudo-spectral solution of nonlinear Schro¨dinger equations
Journal of Computational Physics
Approximate solutions to the Zakharov equations via finite differences
Journal of Computational Physics
A conservative difference scheme for the Zhakarov equations
Journal of Computational Physics
Finite difference method for generalized Zakharov equations
Mathematics of Computation
Runge-Kutta methods for hyperbolic conservation laws with stiff relaxation terms
Journal of Computational Physics
Uniformly Accurate Schemes for Hyperbolic Systems with Relaxation
SIAM Journal on Numerical Analysis
Numerical Initial Value Problems in Ordinary Differential Equations
Numerical Initial Value Problems in Ordinary Differential Equations
On time-splitting spectral approximations for the Schrödinger equation in the semiclassical regime
Journal of Computational Physics
SIAM Journal on Scientific Computing
Numerical methods for the generalized Zakharov system
Journal of Computational Physics
Numerical simulation of a generalized Zakharov system
Journal of Computational Physics
Efficient and Stable Numerical Methods for the Generalized and Vector Zakharov System
SIAM Journal on Scientific Computing
Local discontinuous Galerkin methods for the generalized Zakharov system
Journal of Computational Physics
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The generalized Zakharov system (ZS) couples a dispersive field E (scalar or vectorial) and$$\mathcal{J}$$ nondispersive fields$$\{n_j\}_{j=1}^\mathcal{J}$$ with a propagating speed of$$1/\in_j$$. In this paper, we extend our one-dimensional time-splitting spectral method (TSSP) for the generalized ZS into higher dimension. A main new idea is to reformulate the multi-dimensional wave equations for the nondispersive fields into a first-order system using a change of variable defined in the Fourier space. The proposed scheme TSSP is unconditionally stable, second-order in time and spectrally accurate in space. Moreover, in the subsonic regime, it allows numerical capturing of the subsonic limit without resolving the small parameters$$\in_j$$. Numerical examples confirm these properties of this method